A multi-object spectrograph using single-mode fibers with a coronagraph: progress towards laboratory results on the high-contrast testbed for segmented telescopes

Using single-mode fibers (SMFs) in the image plane of coronagraphs allows access to a new wavefront control regime. By using deformable mirrors to create a mismatch between the incoming starlight and the fiber mode, SMFs can serve as integral parts of the light suppression ability of the coronagraph. Previous promising simulation results show increased spectral bandwidth and throughput when using SMFs in a multi-object role, and previous laboratory results have shown increased light suppression using a single SMF. We present an update on efforts to combine a multi-core SMF with a high-resolution spectrograph on the High Contrast Testbed for Segmented Telescopes (HCST) at Caltech. We present our planned experimental design, as well as simulations of expected performance when controlling multiple fiber cores on HCST. We will test the potential increase in spectral bandpass and throughput resulting from the switch to SMFs, as well as the stability of the wavefront control solution.

[1]  Stuart B. Shaklan,et al.  Fast linearized coronagraph optimizer (FALCO) I: a software toolbox for rapid coronagraphic design and wavefront correction , 2018, Astronomical Telescopes + Instrumentation.

[2]  Dimitri Mawet,et al.  Observing Exoplanets with High Dispersion Coronagraphy. I. The Scientific Potential of Current and Next-generation Large Ground and Space Telescopes , 2017, 1703.00582.

[3]  S. Shaklan,et al.  Simulations of a high-contrast single-mode fiber coronagraphic multiobject spectrograph for future space telescopes , 2019, Journal of Astronomical Telescopes, Instruments, and Systems.

[4]  Frantz Martinache,et al.  Laboratory demonstration of Phase Induced Amplitude Apodization (PIAA) coronagraph with better than 10-9 contrast , 2013, Optics & Photonics - Optical Engineering + Applications.

[5]  F. Roddier,et al.  Coupling starlight into single-mode fiber optics. , 1988, Applied optics.

[6]  Robert J. Vanderbei,et al.  Lyot coronagraph design study for large, segmented space telescope apertures , 2016, Astronomical Telescopes + Instrumentation.

[7]  J. Krist,et al.  D-92350 TECHNOLOGY DEVELOPMENT FOR EXOPLANET MISSONS Technology Milestone # 1 Report : Vortex Coronagraph Technology , 2014 .

[8]  Jacques-Robert Delorme,et al.  Demonstration of an electric field conjugation algorithm for improved starlight rejection through a single mode optical fiber , 2019, Journal of Astronomical Telescopes, Instruments, and Systems.

[9]  John E. Krist,et al.  A hybrid Lyot coronagraph for the direct imaging and spectroscopy of exoplanet systems: recent results and prospects , 2011, Optical Engineering + Applications.

[10]  G. Ruane,et al.  Fast linearized coronagraph optimizer (FALCO) IV: coronagraph design survey for obstructed and segmented apertures , 2018, Astronomical Telescopes + Instrumentation.

[11]  S. Ridgway,et al.  Exoplanet Imaging with a Phase-induced Amplitude Apodization Coronagraph. I. Principle , 2004, astro-ph/0412179.

[12]  Jacques-Robert Delorme,et al.  Wavefront control for minimization of speckle coupling into a fiber injection unit based on the electric field conjugation algorithm , 2018, Astronomical Telescopes + Instrumentation.

[13]  Amir Give'on,et al.  Broadband wavefront correction algorithm for high-contrast imaging systems , 2007, SPIE Optical Engineering + Applications.

[14]  W. Traub,et al.  A Coronagraph with a Band-limited Mask for Finding Terrestrial Planets , 2002, astro-ph/0203455.

[15]  R. Vanderbei,et al.  Extrasolar Planet Finding via Optimal Apodized-Pupil and Shaped-Pupil Coronagraphs , 2003 .

[16]  Jacques-Robert Delorme,et al.  Baseline requirements for detecting biosignatures with the HabEx and LUVOIR mission concepts , 2018 .

[17]  Mamadou N'Diaye,et al.  Optimal deformable mirror and pupil apodization combinations for apodized pupil Lyot coronagraphs with obstructed pupils , 2018, Astronomical Telescopes + Instrumentation.

[18]  M. Kenworthy,et al.  The Single-mode Complex Amplitude Refinement (SCAR) coronagraph , 2018, Astronomy & Astrophysics.

[19]  R. Soummer Apodized Pupil Lyot Coronagraphs for Arbitrary Telescope Apertures , 2004, astro-ph/0412221.

[20]  Mamadou N'Diaye,et al.  APODIZED PUPIL LYOT CORONAGRAPHS FOR ARBITRARY APERTURES. V. HYBRID SHAPED PUPIL DESIGNS FOR IMAGING EARTH-LIKE PLANETS WITH FUTURE SPACE OBSERVATORIES , 2016, 1601.02614.

[21]  Dimitri Mawet,et al.  The high-contrast spectroscopy testbed for segmented telescopes (HCST): new wavefront control demonstrations , 2019, Optical Engineering + Applications.

[22]  Jeffrey Jewell,et al.  Apodized vortex coronagraph designs for segmented aperture telescopes , 2016, Astronomical Telescopes + Instrumentation.

[23]  G. Ruane,et al.  High-contrast spectroscopy testbed for Segmented Telescopes: instrument overview and development progress , 2018, Astronomical Telescopes + Instrumentation.

[24]  C. U. Keller,et al.  The Single-mode Complex Amplitude Refinement (SCAR) coronagraph , 2020, Astronomy & Astrophysics.

[25]  Amir Give'on,et al.  Pair-wise, deformable mirror, image plane-based diversity electric field estimation for high contrast coronagraphy , 2011, Optical Engineering + Applications.

[26]  D. Mawet,et al.  Observing Exoplanets with High-dispersion Coronagraphy. II. Demonstration of an Active Single-mode Fiber Injection Unit , 2017, 1703.00583.

[27]  W. Traub,et al.  A laboratory demonstration of the capability to image an Earth-like extrasolar planet , 2007, Nature.

[28]  D. Mawet,et al.  Annular Groove Phase Mask Coronagraph , 2005 .

[29]  G. Swartzlander,et al.  Optical vortex coronagraph. , 2005, Optics letters.

[30]  Brian Kern,et al.  Fast linearized coronagraph optimizer (FALCO) III: optimization of key coronagraph design parameters , 2018, Astronomical Telescopes + Instrumentation.